Turnitin
降AI改写
早检测系统
早降重系统
Turnitin-UK版
万方检测-期刊版
维普编辑部版
Grammarly检测
Paperpass检测
checkpass检测
PaperYY检测
Fast iterative method with a second-order implicit difference scheme for time-space fractional convection–diffusion equation
In this paper we intend to establish fast numerical approaches to solve a class of initial-
boundary problem of time-space fractional convection–diffusion equations. We present a …
boundary problem of time-space fractional convection–diffusion equations. We present a …
Stability and convergence of a new finite volume method for a two-sided space-fractional diffusion equation
In this paper, we consider a two-sided space-fractional diffusion equation with variable
coefficients on a finite domain. Firstly, based on the nodal basis functions, we present a new …
coefficients on a finite domain. Firstly, based on the nodal basis functions, we present a new …
A monotone finite volume method for time fractional Fokker-Planck equations
Y Jiang, X Xu - Science China Mathematics, 2019 - Springer
We develop a monotone finite volume method for the time fractional Fokker-Planck
equations and theoretically prove its unconditional stability. We show that the convergence …
equations and theoretically prove its unconditional stability. We show that the convergence …
Computational challenge of fractional differential equations and the potential solutions: a survey
We present a survey of fractional differential equations and in particular of the computational
cost for their numerical solutions from the view of computer science. The computational …
cost for their numerical solutions from the view of computer science. The computational …
A finite volume method for two-sided fractional diffusion equations on non-uniform meshes
We derive a finite volume method for two-sided fractional diffusion equations with Riemann–
Liouville derivatives in one spatial dimension. The method applies to non-uniform meshes …
Liouville derivatives in one spatial dimension. The method applies to non-uniform meshes …
A parallel algorithm for the Riesz fractional reaction-diffusion equation with explicit finite difference method
C Gong, W Bao, G Tang - Fractional Calculus and Applied Analysis, 2013 - degruyter.com
The fractional reaction-diffusion equations play an important role in dynamical systems.
Indeed, it is time consuming to numerically solve differential fractional diffusion equations. In …
Indeed, it is time consuming to numerically solve differential fractional diffusion equations. In …
[HTML][HTML] Finite element error analysis of a time-fractional nonlocal diffusion equation with the Dirichlet energy
A time-fractional diffusion equation involving the Dirichlet energy is considered with nonlocal
diffusion operator in the space which has dimension d∈{2, 3} and the Caputo sense …
diffusion operator in the space which has dimension d∈{2, 3} and the Caputo sense …
A simulation expressivity of the quenching phenomenon in a two-sided space-fractional diffusion equation
L Zhu, N Liu, Q Sheng - Applied Mathematics and Computation, 2023 - Elsevier
The aims of this paper are to investigate and propose a numerical approximation for a
quenching type diffusion problem associated with a two-sided Riemann-Liouville space …
quenching type diffusion problem associated with a two-sided Riemann-Liouville space …
A unified spectral method for FPDEs with two-sided derivatives; part I: a fast solver
We develop a unified Petrov–Galerkin spectral method for a class of fractional partial
differential equations with two-sided derivatives and constant coefficients of the form D t 2 τ 0 …
differential equations with two-sided derivatives and constant coefficients of the form D t 2 τ 0 …
Finite Volume Methods for N-Dimensional Time Fractional Fokker–Planck Equations
S Zhou, Y Jiang - Bulletin of the Malaysian Mathematical Sciences …, 2019 - Springer
We develop a finite volume method to numerically solve the N-dimensional time fractional
Fokker–Planck equation ∂^ α ω ∂ t^ α= k_ α Δ ω-∑\limits _ k= 1^ N ∂ (f^(k) ω) ∂ x_k,∂ α …
Fokker–Planck equation ∂^ α ω ∂ t^ α= k_ α Δ ω-∑\limits _ k= 1^ N ∂ (f^(k) ω) ∂ x_k,∂ α …